ISEE 1 and 2 observations of ion distributions at the plasma sheet‐tail lobe boundary

Observations of plasma ions (0.075–29 keV) at or near the plasma sheet-tail lobe boundary made with the ISEE 1 and 2 spacecraft are the principal topic of this paper. We describe crossings of this boundary that occurred during various levels of geomagnetic activity at distances XSM = −7 to −13 RE, near local midnight, and 2 RE or more above the estimated location of the tail current sheet. Fluxes of ions directed along the magnetic field lines (referred to as ion beams) with kinetic energies of 1- > 29 keV are commonly observed during crossings of this boundary. The ion beams nearest the edge of the plasma sheet are directed earthward, while deeper within the plasma sheet, additional ion beams, directed tailward, are encountered, usually resulting in bidirectional or counterstreaming ion distributions. The ion distribution functions for these clearly indicate that the tailward directed beams are reflected versions of the earthward directed beams, returning after mirroring in the stronger magnetic field near the Earth. From an intersatellite timing analysis the thickness dB of the region of solely earthward streaming ions is estimated to be a few tenths of an Earth radius. The fastest particles (plasma electrons and the highest-energy ions) are the first to be seen as a satellite enters the plasma sheet from the lobe and last to be seen as it leaves the plasma sheet to enter the lobe. This suggests that the ion beams are components of a layer of plasma that is projected earthward along field lines from a more or less steady source tailward of the satellite and that is E × B drifting equatorward. The observations are consistent with theoretical predictions for an open model of the magnetosphere having a neutral line tailward of the satellite and having the plasma sheet-lobe interface coincident with the separatrix between closed and open field lines. We therefore identify the beam-containing plasma layer contiguous to, and extending equatorward from, this interface as the separatrix layer. The velocity, temperature, and kinetic energy flux of the earthward beams in the separatrix layer are found to correlate positively with the AE index. We rarely observe isolated tailward streaming ion beams near the boundary, although slow (<300 km/s) tailward flows there sometimes result from an imbalance of particle fluxes carried by the oppositely streaming beams. We show that such net tailward ion anisotropies, occasionally observed in our data set, differ distinctly from the tailward bulk flow event reported by Hones et al. (1986). That event had all ion components moving tailward with a net velocity of ∼500 km/s; it was interpreted to be the result of magnetic reconnection at a near-Earth neutral line that formed at the onset of a substorm and tailward departure of the resulting plasmoid.

[1]  E. W. Hones,et al.  Multiple crossings of a very thin plasma sheet in the Earth's magnetotail , 1981 .

[2]  E. W. Hones,et al.  Associations of geomagnetic activity with plasma sheet thinning and expansion: A statistical study , 1984 .

[3]  T. Eastman,et al.  The plasma sheet boundary layer , 1983 .

[4]  W. I. Axford,et al.  Energetic protons near the plasma sheet boundary , 1979, Nature.

[5]  E. W. Hones,et al.  On the velocity distribution of ion jets during substorm recovery , 1981 .

[6]  T. Eastman,et al.  Observations of ion streaming during substorms , 1983 .

[7]  E. W. Hones,et al.  Substorm variations of the magnetotail plasma sheet from X SM ≈ −6 RE to X SM ≈ −60 RE , 1973 .

[8]  C. Huang,et al.  A statistical study of the central plasma sheet: Implications for substorm models , 1986 .

[9]  E. W. Hones,et al.  Evolution of the Earth's distant magnetotail: ISEE 3 electron plasma results , 1984 .

[10]  E. W. Hones,et al.  Magnetotail plasma flow measured by Vela 4A , 1973 .

[11]  M. K. Andrews,et al.  Plasma sheet motions inferred from medium-energy ion measurements , 1981 .

[12]  D. A. Bryant,et al.  Auroral electron acceleration by lower-hybrid waves , 1985 .

[13]  C. Russell,et al.  Some remarks on the position and shape of the neutral sheet , 1967 .

[14]  E. W. Hones,et al.  Substorm‐related plasma sheet motions as determined from differential timing of plasma changes at the Isee satellites , 1981 .

[15]  L. M. Chase,et al.  Magnetotail electric fields observed from lunar orbit , 1975 .

[16]  D. Evans An Association Between Discrete Aurora and Energetic Particle Boundaries L. R. LYONS Space Science Laboratory, NASA Marshall Space Flight Center , 1984 .

[17]  T. Eastman,et al.  Particle and field characteristics of the high-latitude plasma sheet boundary layer , 1984 .

[18]  E. W. Hones Substorm processes in the magnetotail - Comments on 'On hot tenuous plasmas, fireballs, and boundary layers in the earth's magnetotail' by L. A. Frank, K. L. Ackerson, and R. P. Lepping , 1977 .

[19]  E. W. Hones,et al.  On the three-dimensional magnetic structure of the plasmoid created in the magnetotail at substorm onset , 1982 .

[20]  B. Klecker,et al.  Fast moving plasma structures in the distant magnetotail , 1984 .

[21]  F. Mozer,et al.  Observations of large electric fields near the plasmasheet boundary by ISEE-1 , 1982 .

[22]  H. Matsumoto,et al.  Particle acceleration in time‐developing magnetic reconnection process , 1982 .

[23]  E. W. Hones,et al.  Measurements of magnetotail plasma flow made with Vela 4B , 1972 .

[24]  D. Williams,et al.  Sources for energetic ions at the plasma sheet boundary: Time varying or steady state? , 1984 .

[25]  E. W. Hones,et al.  Magnetotail plasma flow during plasma sheet expansions: Vela 5 and 6 and Imp 6 observations , 1977 .

[26]  E. W. Hones,et al.  Three‐dimensional computer modeling of dynamic reconnection in the geomagnetic tail , 1981 .

[27]  E. W. Hones,et al.  Detailed examination of a plasmoid in the distant magnetotail with ISEE 3 , 1984 .

[28]  E. W. Hones,et al.  Outward flow of plasms in the magnetotail following geomagnetic bays , 1967 .

[29]  E. W. Hones,et al.  Structure of the magnetotail at 220 RE and its response to geomagnetic activity , 1984 .

[30]  S. Cowley Plasma populations in a simple open model magnetosphere , 1980 .

[31]  M. K. Andrews,et al.  Ion jetting at the plasma sheet boundary: simultaneous observations of incident and reflected particles , 1981 .

[32]  H. Rosenbauer,et al.  ISEE-1 and ISEE-2 Fast Plasma Experiment and the ISEE-1 Solar Wind Experiment , 1978, IEEE Transactions on Geoscience Electronics.

[33]  E. W. Hones,et al.  Detailed observations of the plasma sheet during a substorm on April 24, 1979 , 1986 .

[34]  E. W. Hones,et al.  Plasmoid-associated energetic ion bursts in the deep geomagnetic tail: Properties of plasmoids and the postplasmoid plasma sheet , 1987 .

[35]  T. Speiser,et al.  Evidence for current sheet acceleration in the geomagnetic tail , 1982 .

[36]  V. Vasyliūnas Theoretical models of magnetic field line merging , 1975 .

[37]  Tetsuya Sato,et al.  Generation of large scale potential difference by currentless plasma jets along the mirror field , 1984 .

[38]  E. W. Hones,et al.  Gradients of solar protons in the high-latitude magnetotail and the magnetospheric electric field , 1976 .

[39]  L. Frank,et al.  Observations pertaining to the dynamics of the plasma sheet. [in geomagnetic tail] , 1977 .

[40]  S. Krimigis,et al.  Observations of magnetospheric bursts of high-energy protons and electrons at ∼35 RE with Imp 7 , 1976 .

[41]  D. Williams Phase space variations of near equatorially mirroring ring current ions , 1981 .

[42]  E. W. Hones,et al.  Time variations of the magnetotail plasma sheet at 18 RE Determined from concurrent observations by a pair of Vela satellites , 1971 .

[43]  J. Sauvaud,et al.  A statistical study of plasma sheet dynamics using Isee 1 and 2 energetic particle flux data , 1986 .

[44]  T. Fritz,et al.  Energetic ion and electron observations of the geomagnetic plasma sheet boundary layer: Three‐dimensional results from Isee 1 , 1981 .

[45]  J. Kan Energization of auroral electrons by electrostatic shock waves , 1975 .

[46]  E. W. Hones,et al.  Proton flow measurements in the magnetotail plasma sheet made with Imp 6 , 1976 .

[47]  E. W. Hones,et al.  Evidence for the tailward retreat of a magnetic neutral line in the magnetotail during substorm recovery , 1981 .

[48]  T. Eastman,et al.  The boundary layers as the primary transport regions of the earth's magnetotail , 1985 .

[49]  C. Russell,et al.  Observations of field‐aligned currents at the plasma sheet boundary: An ISEE‐1 and 2 survey , 1985 .

[50]  E. Möbius,et al.  Observations of a nonthermal ion layer at the plasma sheet boundary during substorm recovery , 1980 .

[51]  E. W. Hones,et al.  Field‐aligned plasma flow in MHD simulations of magnetotail reconnection and the formation of boundary layers , 1986 .

[52]  G. Parks,et al.  ISEE 1 and 2 particle observations of outer plasma sheet boundary , 1979 .

[53]  M. Scholer Earthward plasma flow during near‐Earth magnetotail reconnection: Numerical simulations , 1987 .

[54]  J. Birn,et al.  On the generation of field-aligned plasma flow at the boundary of the plasma sheet , 1987 .

[55]  E. W. Hones,et al.  Magnetotail plasma flow during substorms: A survey with Imp 6 and Imp 8 satellites , 1979 .

[56]  T. Eastman,et al.  High-altitude observations of an intense inverted-V event. Report for period ending May 78 , 1984 .

[57]  D. Williams Energetic ion beams at the edge of the plasma sheet: ISEE 1 observations plus a simple explanatory model , 1981 .